Motor control device and compressor

ABSTRACT

A motor control device performing vector control for a motor that drives a load whose load torque varies periodically. The motor control device has: a motor speed deriving portion estimating or detecting a motor speed; a speed controller producing a specified torque current value such that the motor speed is made to follow a specified motor speed value fed from outside; a resonance filter producing a corrected torque current value by receiving a control value that varies with variations in the load torque and emphasizing a periodic variation component of the control value; a torque current corrector producing a specified superimposed torque current value by superimposing the corrected torque current value on the specified torque current value; and an adjusting portion adjusting, based on the specified superimposed torque current value, a degree of emphasis placed on the variation component by the resonance filter. The vector control is performed according to the specified superimposed torque current value.

This nonprovisional application claims priority under 35 U.S.C. §119(a) on Patent Application No. 2007-165059 filed in Japan on Jun. 22, 2007, the entire contents of which are hereby incorporated by reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to motor control devices that control a motor and to compressors.

2. Description of Related Art

A load factor of a motor often entails periodic load variations. A compressor used in an air conditioner or the like is an example of a product including such a load factor. In a hermetic type compressor used in an air conditioner, a change in refrigerant gas pressure during cycles of suction, compression, and discharge is known to affect a load torque. It is also known that the load torque associated with the refrigerant gas pressure varies in synchronism with the rotation of the compressor, resulting in periodic variations in rotation speed of the compressor. Such periodic variations in rotation speed of the compressor produce vibration in the compressor itself, and also cause noise.

To solve the problems such as vibration and noise caused by variations in load torque, various methods have been proposed. For example, there has been proposed a conventional method adopting torque control that estimates a variation component of a torque produced by a load device and compensates for the variation component thus estimated, wherein a current component for compensating for the variation component is limited by a limit value.

For example, in another conventional method, a torque variation component is extracted based on, for example, the deviation of the estimated motor speed from the specified motor speed value, and the extracted torque variation component is used to reduce vibration.

In addition to reducing vibration and noise of a device, reducing power consumption in a system for driving a motor is an important problem to be solved.

SUMMARY OF THE INVENTION

According to one aspect of the present invention, a motor control device performing vector control for a motor that drives a load whose load torque varies periodically is provided with: a motor speed deriving portion estimating or detecting a motor speed; a speed controller producing a specified torque current value such that the motor speed is made to follow a specified motor speed value fed from outside; a resonance filter producing a corrected torque current value by receiving a control value that varies with variations in the load torque and emphasizing a periodic variation component of the control value; a torque current corrector producing a specified superimposed torque current value by superimposing the corrected torque current value on the specified torque current value; and an adjusting portion adjusting, based on the specified superimposed torque current value, a degree of emphasis placed on the variation component by the resonance filter. Here, the vector control is performed according to the specified superimposed torque current value.

Specifically, for example, the control value is the difference between the motor speed and the specified motor speed value, or the control value is the specified torque current value.

Preferably, for example, let an axis parallel to a magnetic flux produced by a permanent magnet provided on a rotor of the motor be called a d-axis, and let an axis estimated for control purposes, the axis corresponding to the d-axis, be called a γ-axis. Then, the motor control device includes an estimator estimating, based on a motor current to be fed to the motor, an axis error between the d-axis and the γ-axis, and the motor speed. Here, the control value is the axis error, or a value varying in synchronism with variations in the axis error.

Specifically, for example, the adjusting portion adjusts the degree of emphasis based on a variation range of the specified superimposed torque current value.

Preferably, for example, the adjusting portion adjusts the degree of emphasis such that the variation range is reduced.

Preferably, for example, the adjusting portion extracts, from the specified superimposed torque current value, a frequency component of variations in the load torque, and adjusts the degree of emphasis based on the amplitude of the frequency component.

Preferably, for example, the adjusting portion adjusts the degree of emphasis such that the amplitude of the frequency component is reduced.

According to another aspect of the present invention, a motor drive system is provided with: a motor; an inverter driving the motor; and the motor control device described above, the motor control device performing vector control for the motor via the inverter.

According to still another aspect of the present invention, a compressor uses, as a drive source thereof, a torque of the motor provided in the motor drive system described above.

The significance and effect of the present invention will become more apparent from the following detailed description of an embodiment thereof. It is to be understood that the significance of the present invention and the significance of terms describing the component elements thereof are not limited in any way by those specifically described in the embodiment below, because the embodiment below is merely an example of how the invention can be implemented.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a schematic block diagram of a motor drive system embodying the invention;

FIG. 2 is an analysis model diagram of the motor shown in FIG. 1;

FIG. 3 is a detailed block diagram of a motor drive system according to Example 1 of the invention;

FIG. 4 is an internal block diagram of the position/speed estimator shown in FIG. 3;

FIG. 5 is a diagram according to Example 1 of the invention, showing the waveforms of a current conversion value of a load torque, a specified δ-axis current value, an error between the current conversion value of a load torque and the specified δ-axis current value, and a corrected δ-axis current value;

FIG. 6A is a diagram showing gain characteristics of the resonance filter shown in FIG. 3;

FIG. 6B is a diagram showing phase characteristics of the resonance filter shown in FIG. 3;

FIG. 7 is a diagram showing the measurement results of the variation range of (i_(δ)*+i_(δC)), the amplitude of a first-order component of (i_(δ)*+i_(δC)), and the amount of decrease or increase of power consumption, the measurement results being obtained when the gain of the resonance filter shown in FIG. 3 is variously changed;

FIG. 8 is a diagram showing the FFT analysis results of (i_(δ)*+i_(δC)) inputted to the gain controller shown in FIG. 3;

FIG. 9 is an enlarged view of part of FIG. 8, showing the FFT analysis results of (i_(δ)*+i_(δC)) inputted to the gain controller shown in FIG. 3;

FIG. 10 is a flow chart showing the procedure for minimizing the variation range of (i_(δ)*+i_(δC)) inputted to the gain controller shown in FIG. 3;

FIG. 11 is a detailed block diagram of a motor drive system according to Example 2 of the invention;

FIG. 12 is a detailed block diagram of a motor drive system according to Example 3 of the invention;

FIG. 13 is an external view of a compressor driven by the motor drive system of the invention; and

FIG. 14 is a diagram showing the simulation results according to Example 7 of the invention.

DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS

Hereinafter, the present invention will be described by way of a specific embodiment with reference to the accompanying drawings. Among these drawings, such parts that appear more than once are identified with common reference designations, and in principle the description of any part, once given, will not be repeated. First, matters common to Examples 1 to 7, which will be described later, or matters to which reference is made in these examples will be described.

FIG. 1 is a schematic block diagram of a motor drive system embodying the invention. The motor drive system shown in FIG. 1 includes a motor 1, a PWM (pulse width modulation) inverter 2, and a motor control device 3.

The motor 1 is a three-phase permanent-magnet synchronous motor provided with a rotor (unillustrated) having a permanent magnet and a stator (unillustrated) having armature windings, one for each of three phases.

The PWM inverter (hereinafter referred to simply as the “inverter”) 2 supplies three-phase alternating-current voltages, consisting of U-phase, V-phase, and W-phase voltages, to the motor 1 according to the rotor position of the motor 1. These voltages supplied to the motor 1 are collectively referred to as the motor voltage (armature voltage) V_(a), and the currents supplied from the inverter 2 to the motor 1 are collectively referred to as the motor current (armature current) I_(a).

The motor control device 3 feeds the inverter 2 with a PWM signal for achieving desired vector control while referring to the detected motor current I_(a) or the like.

FIG. 2 is an analysis model diagram of the motor 1. In the following description, what is referred to simply by the “armature winding” should be understood to mean the armature winding provided on the motor 1. FIG. 2 shows the U-phase, V-phase, and W-phase armature winding fixed axes. Reference numeral 1 a represents the permanent magnet constituting the rotor of the motor 1. In a rotating coordinate system that rotates at the same speed as the magnetic flux produced by the permanent magnet 1 a, the direction of the magnetic flux produced by the permanent magnet 1 a is referred to as the d-axis, and the rotation axis for control purposes, the rotation axis corresponding to the d-axis, is referred to as the γ-axis. Though not illustrated, the axis having a phase leading the d-axis by an electrical angle of 90 degrees is referred to as the q-axis, and the axis having a phase leading the γ-axis by an electrical angle of 90 degrees is referred to as the δ-axis. The rotating coordinate system corresponding to the real axes has the d- and q-axes as its coordinate axes, and its coordinate axes are called the d-q axes. The rotating coordinate system for control purposes has the γ- and δ-axes as its coordinate axes, and its coordinate axes are called the γ-δ axes.

The d-q axes rotates, and its rotation speed is represented by ω. The γ-δ axes also rotates, and its rotation speed is represented by ω_(e). With respect to the d-q axes, the angle (phase) of the d-axis is represented, relative to the U-phase armature winding fixed axis, by θ. Likewise, with respect to the γ-δ axes, the angle (phase) of the γ-axis is represented, relative to the U-phase armature winding fixed axis, by θ_(e). The angle represented by θ or θ_(e) is the angle in electrical angle, and is commonly referred to as a rotor position or a magnetic pole position. The rotation speed represented by ω_(e) or ω_(e) is the angular velocity at electrical angle.

Hereinafter, θ or θ_(e) is referred to as a rotor position, and ω or ω_(e) is referred to as a motor speed. In a case where the rotor position and the motor speed are derived by estimation, as in Example 1 or the like, which will be described later, the γ- and δ-axes can be called the axes estimated for control purposes.

Although the motor control device 3 basically performs vector control such that θ becomes equal to θ_(e), it sometimes intentionally makes θ different from θ_(e). When θ is equal to θ_(e), the d-axis and the q-axis are equal to the γ-axis and the δ-axis, respectively.

In the following description, the γ-axis component and the δ-axis component of the motor voltage V_(a) are referred to as the γ-axis voltage v_(γ) and the δ-axis voltage v_(δ), respectively, and the γ-axis component and the δ-axis component of the motor current I_(a) are referred to as the γ-axis current i_(γ) and the δ-axis current i_(δ), respectively.

The specified voltage values, or target values, of the γ-axis voltage v_(γ) and the 6-axis voltage v_(δ) are referred to as the specified γ-axis voltage value v_(γ)* and the specified δ-axis voltage value v_(δ)*, respectively. The specified current values, or target values, of the γ-axis current i_(γ) and the δ-axis current i_(δ) are referred to as the specified γ-axis current value i_(γ)* and the specified δ-axis current value i_(δ)*, respectively. Here, v_(γ)* can be called a target γ-axis voltage of v_(γ), and v_(δ)* can be called a target δ-axis voltage of v_(δ); i_(γ)* can be called a target γ-axis current of i_(γ), and i_(δ)* can be called a target δ-axis current of i_(δ).

The motor control device 3 performs vector control such that the values of γ-axis voltage v_(γ) and δ-axis voltage v_(δ) are made to follow the specified γ-axis voltage value v_(γ)* and the specified δ-axis voltage value v_(δ)*, respectively, and such that the values of γ-axis current i_(γ) and δ-axis current is are made to follow the specified γ-axis current value i_(γ)* and the specified δ-axis current value i_(δ)*, respectively.

U-, V-, and W-phase components of the motor voltage V_(a) are represented by the specified three-phase voltage values consisting of a specified U-phase voltage value v_(u)*, a specified V-phase voltage value v_(v)*, and a specified W-phase voltage value v_(w)*.

In the following description, R_(a) represents the motor resistance (the resistance value of the armature winding of the motor 1), and L_(d) and L_(q) represent the d-axis inductance (the d-axis component of the inductance of the armature winding of the motor 1) and the q-axis inductance (the q-axis component of the inductance of the armature winding of the motor 1), respectively. The values of R_(a), L_(d), and L_(q) are determined at the time of fabrication of the motor drive system, and are used by the motor control device 3 to perform calculations.

In the present specification, to make the description simple, state quantities and the like are often referred to by their symbols (such as i_(γ)) alone; for example, the “γ-axis current i_(γ)” is sometimes referred to simply by “i_(γ)” and these should be understood to represent the same thing. In addition, the terms representing the state quantities, such as “current”, “voltage”, and “speed”, represent in principle the values of these state quantities. That is, for example, the “γ-axis current i_(γ)” means the current value of the γ-axis current (however, the wording such as “the value of the γ-axis current i_(γ)” may be sometimes used).

The motor 1 drives and rotates a load whose load torque varies periodically. This load is, for example, a load factor provided in a compressor (see FIG. 13), a washing machine (unillustrated), a drying machine (unillustrated), or the like. The compressor is used in an air conditioner or the like. In the compressor, a change in refrigerant gas pressure during periodic cycles of suction, compression, and discharge affects a load torque, resulting in periodic variations in load torque.

Specifically, the washing machine or the drying machine is, for example, a drum washing machine or a drum drying machine. In the drum washing machine, a drum inside which laundry is placed rotates about a rotation axis that is not parallel to the vertical line, such that the laundry is lifted up and then dropped to remove a stain. In a case where the drum is a load of the motor 1, the load torque becomes relatively large when the laundry is lifted up; otherwise it becomes relatively small. This results in periodic variations in load torque. The same holds true for the drum drying machine.

Example 1

First, Example 1 of the invention will be described. FIG. 3 is a detailed block diagram of a motor drive system according to Example 1. The motor drive system shown in FIG. 3 includes the motor 1 and the inverter 2 shown in FIG. 1, a motor control device 3 a serving as the motor control device 3 shown in FIG. 1, and a phase-current sensor 11. The motor control device 3 a includes different parts designated with reference numerals 12 to 20 and 30 to 32. The motor control device 3 a can be considered to include the phase-current sensor 11. The different parts constituting the motor control device 3 a can freely use all the values produced within the motor control device 3 a.

The different parts constituting the motor drive systems of this example and other examples, which will be described later, update, at intervals of a predetermined period, the specified values (including i_(γ)*, i_(δ)*, v_(γ)*, v_(δ)*, v_(u)*, v_(v)*, and v_(w)*), the state quantities (including i_(u), i_(v), i_(γ), i_(δ), θ_(e), and ω_(e)), or the corrected δ-axis current value i_(δC), which are calculated (or detected) thereby and outputted therefrom.

The phase-current sensor 11 detects a U-phase current i_(u) and a V-phase current i_(v) which are the fixed-axis components of the motor current I_(a) supplied from the inverter 2 to the motor 1. It is to be noted that a W-phase current i_(w) is calculated by using the following relational expression: i_(w)=−i_(u)−i_(v). Here, i_(u), i_(v), and i _(w) are currents of the U-, V-, and W-phase armature windings, respectively, of the stator of the motor 1.

The coordinate converter 12 performs coordinate conversion based on the rotor position θ_(e) so that the U-phase current i_(u) and the V-phase current i_(v) are converted into those on the γ-δ axes, and thereby calculates the γ-axis current i_(γ) and the δ-axis current i_(δ) and outputs them. In Example 1, the rotor position θ_(e) is calculated by the position/speed estimator 20.

The subtracter 19 refers to the motor speed ω_(e) and the specified motor speed value ω* from a specified motor speed value producing portion (unillustrated) provided outside the motor control device 3 a, and calculates the speed deviation (ω*−ω_(e)) between them. In Example 1, the motor speed ω_(e) is calculated by the position/speed estimator 20.

The speed controller 17 calculates the specified δ-axis current value i_(δ)* by using proportional-plus-integral control or the like, such that the speed deviation (ω*−ω_(e)) converges to zero, and outputs the specified δ-axis current value i_(δ)* thus calculated. The adder 31 adds the corrected δ-axis current value i_(δC) from the resonance filter 30 to i_(δ)* from the speed controller 17, and outputs the value (i_(δ)*+i_(δC)) obtained by the addition to the subtracter 13. The value (i_(δ)*+i_(δC)) is also given to the gain controller 32. Originally, is serves as a target value of is; in actuality, the value (i_(δ)*+i_(δC)) obtained by correcting is with the resonance filter 30 and the adder 31 serves as a target value of i_(δ). Operations of the resonance filter 30 and the gain controller 32 will be described later.

The magnetic flux controller 16 determines the specified γ-axis current value i_(γ)*, and outputs it to the subtracter 14. Here, i_(γ)* can take on different values in accordance with the type of vector control performed in the motor drive system and the motor speed. In this example, the d-q axes are estimated. Therefore, in a case where control for making the d-axis current equal to zero is performed, i_(γ)*=0 holds. In a case where maximum torque control or flux-weakening control is performed, i_(γ)* takes on a negative value commensurate with the motor speed ω_(e). The operations of the resonance filter 30 and the gain controller 32, which are distinctive parts of the motor control device 3 a, do not depend on the value of i_(γ)*. The following description deals with a case in which i_(γ)*=0.

The subtracter 14 subtracts the γ-axis current i_(γ) outputted from the coordinate converter 12 from the specified γ-axis current value i_(γ) outputted from the magnetic flux controller 16, and thereby calculates the current error (i_(γ)*−i_(γ)). The subtracter 13 subtracts the δ-axis current i_(δ) outputted from the coordinate converter 12 from the value (i_(δ)*+i_(δC)) outputted from the adder 31, and thereby calculates the current error (i_(δ)*+i_(δC)−i_(δ)).

The current controller 15 performs current feedback control by using proportional-plus-integral control or the like, such that the current errors (i_(γ)*−i_(γ)) and (i_(δ)*+i_(δC)−i_(δ)) converge to zero. At this point, the specified γ-axis voltage value v_(γ)* and the specified δ-axis voltage value v_(δ)* are calculated by using decoupling control for eliminating interference between the γ- and δ-axes, such that (i_(γ)*−i_(γ)) and (i_(δ)*+i_(δC)−i_(δ)) converge to zero. It is to be noted that ω_(e), i_(γ), and i_(δ) can also be referred to at the time of calculation of v_(γ)* and v_(δ)*.

The coordinate converter 18 performs coordinate conversion based on the rotor position θ_(e) outputted from the position/speed estimator 20 so that v_(γ)* and v_(δ)* fed from the current controller 15 are converted into those on the three-phase fixed coordinate axes, and thereby calculates the specified three-phase voltage values (v_(u)*, v_(v)*, and v_(w)*) and outputs them.

An unillustrated PWM converter produces a PWM signal subjected to pulse width modulation in accordance with the specified three-phase voltage values (v_(u)*, v_(v)*, and v_(w)*). The inverter 2 supplies the motor current I_(a) corresponding to the PWM signal to the motor 1 to drive it. More specifically, the inverter 2 includes three half-bridge circuits provided one for each of three phases and a driver, all of which are not shown in the drawing, and the driver performs on/off control for the switching devices of the half-bridge circuits in accordance with the PWM signal, such that the motor current I_(a) according to the specified three-phase voltage values is supplied to the motor 1. The PWM converter is provided in the motor control device 3 a; however, it can be considered to be provided in the inverter 2.

The position/speed estimator 20 performs proportional-plus-integral control or the like by using all or part of i_(γ) and i_(δ) from the coordinate converter 12 and v_(γ)* and v_(δ)* from the current controller 15, and thereby estimates the rotor position θ_(e) and the motor speed ω_(e) such that the axis error Δθ (see FIG. 2; Δθ=θ−θ_(e)) between the d-axis and the 7-axis converges to zero. There have conventionally been proposed various methods for estimating the rotor position θ_(e) and the rotation speed ω_(e), and any method heretofore known can be adopted in the position/speed estimator 20.

FIG. 4 shows an example of an internal block diagram of the position/speed estimator 20. The position/speed estimator 20 shown in FIG. 4 includes different parts designated with reference numerals 21 to 23. The axis error estimator 21 calculates the axis error Δθ based on i_(γ), i_(δ), v_(γ)*, and v_(δ)*. For example, the axis error Δθ is calculated by using formula (1) below, which is disclosed also in JP-B-3411878. To achieve PLL (phase locked loop) control, the proportional-plus-integral calculator 22 performs proportional-plus-integral control to calculate the motor speed ω_(e) such that the axis error Δθ calculated by the axis error estimator 21 converges to zero. The integrator 23 integrates the motor speed ω_(e), and thereby calculates the rotor position ω_(e). The calculated θ_(e) and ω_(e) are fed to different parts of the motor control device 3 a that need them.

$\begin{matrix} {{\Delta\theta} = {\tan^{- 1}\left( \frac{- \left( {v_{\gamma}^{*} - {R_{a}i_{\gamma}} + {\omega_{e}L_{q}i_{\delta}}} \right)}{v_{\delta}^{*} - {R_{a}i_{\delta}} - {\omega_{e}L_{q}i_{\gamma}}} \right)}} & (1) \end{matrix}$

As described above, in this embodiment, it is assumed that the motor 1 drives and rotates a load whose load torque varies periodically. As a result, is may deviate from the ideal value due to variations in load torque. However, the resonance filter 30 and the adder 31 operate so as to prevent such a deviation.

With reference to FIG. 5 and other drawings, the principle of preventing such a deviation will be explained. In FIG. 5, the horizontal axis represents the phase of current in electrical angle, and the vertical axis represents the current value. Since the phase of current changes with time during normal rotation of the motor 1, the horizontal axis of FIG. 5 also represents time. In FIG. 5, a curve 201 represents the current conversion value (current component) of a load torque, a curve 202 represents the specified δ-axis current value i_(δ)* calculated by the speed controller 17, and a curve 203 represents a waveform of error between the current conversion value of a load torque represented by the curve 201 and the specified δ-axis current value i_(δ)* represented by the curve 202. A curve 204 represents a waveform obtained by inverting the waveform of error represented by the curve 203, and also represents a waveform of the corrected δ-axis current value i_(δC) calculated by the resonance filter 30.

To make the motor 1 produce a torque identical to a load torque, it is necessary simply to pass the δ-axis current i_(δ) corresponding to the current conversion value of a load torque. Assume that no corrected δ-axis current value i_(δC) is present. Then, if the current conversion value of a load torque is identical to i_(δ), it is possible to suppress variations in speed caused by variations in load torque, and to reduce vibration and noise.

In actuality, however, due to delay in the control system, the specified δ-axis current value i_(δ)* lags behind the value required to be calculated (the current conversion value of a load torque). To deal with this problem, in this example, the corrected δ-axis current value i_(δC) corresponding to the curve 204 is superimposed on i_(δ)*, such that (i_(δ)*+i_(δC)) is made identical to the current conversion value of a load torque. To make (i_(δ)*+i_(δC)) identical to the current conversion value of a load torque requires the optimization of the phase and amplitude of i_(δC). In this example, the gain controller 32 (FIG. 3) is used to make adjustment for the optimization of the amplitude. The function of the gain controller 32 is described later. First, the function of the resonance filter 30 will be described.

The resonance filter 30 receives a subtraction result (ω*−ω_(e)) of the subtracter 19 as an input signal, and extracts from the input signal thus received a periodic variation component resulting from variations in load torque. Then, the resonance filter 30 outputs the extracted variation component as i_(δC). The transfer function H_(A)(s) of the resonance filter 30 is given by formula (2) below (or formula (3), which will be described later). H _(A)(s)=(b ₀ +b ₁ s)/(s ²+2ζω_(r) s+ω _(r) ²)  (2)

Here, b₀ represents a gain coefficient, b₁ represents a phase adjusting value, ζ represents an attenuation coefficient, and ω_(r) represents a natural angular frequency. In addition, s represents the Laplace operator. Ideally, the resonance filter 30 extracts only a frequency component of ω_(r) of the input signal, and outputs it.

FIG. 6A shows the gain characteristics of the resonance filter 30. The resonance filter 30 amplifies (emphasizes) a component of natural angular frequency ω_(r) contained in the input signal to a degree commensurate with the gain coefficient b₀, and outputs it. At this time, the resonance filter 30 makes the output signal contain as few as possible a frequency component other than ω_(r). FIG. 6B shows the phase characteristics of the resonance filter 30. The resonance filter 30 gives the component of natural angular frequency ω_(r) 90 degrees phase lead, and gives a component having a frequency lower than the natural angular frequency ω_(r) 180 degrees phase lead. The phase of a component having a frequency higher than the natural angular frequency ω_(r) is identical between the input and output signals of the resonance filter 30.

The natural angular frequency ω_(r) is set so as to be identical (or as identical as possible) to the angular frequency of periodic load torque variations of the load of the motor 1. The value of the natural angular frequency ω_(r) is made to change according to the specified motor speed value ω* or the value of the motor speed ω_(e), because the period of the load torque variations changes according to the rotational speed of the motor 1. How to set the natural angular frequency ω_(r) according to the specified motor speed value ω* or the value of the motor speed ω_(e) is previously defined at the design stage of the motor drive system. For example, the motor control device 3 a is previously provided with the table data for determining ω_(r) based on ω* or ω_(e).

The attenuation coefficient ζ is a value for determining the degree of resonance (resonance characteristics) of the resonance filter 30, and can take on any value as long as 0≦ζ<1. For example, ζ=0.01 or Λ=0.1. The attenuation coefficient ζ can be previously determined at the design stage of the motor drive system.

The phase adjusting value b₁ is a value for adjusting the phase of the corrected δ-axis current value i_(δC). Changing the phase adjusting value b₁ causes the curve 204 shown in FIG. 5 to shift in the horizontal direction. The phase adjusting value b₁ changes according to the specified motor speed value ω* or the value of the motor speed ω_(e). How to set the phase adjusting value b₁ according to the specified motor speed value ω* or the value of the motor speed ω_(e) is previously defined at the design stage of the motor drive system. For example, the motor control device 3 a is previously provided with the table data for determining b₁ based on ω* or ω_(e). If there is no need to adjust the phase of i_(δC) with the resonance filter 30, b₁=0.

The gain of the resonance filter 30, that is, the degree of emphasis placed on the component of natural angular frequency ω_(r) contained in the input signal of the resonance filter 30, is determined by the gain coefficient b_(o). More specifically, if b₁=0, the gain of the resonance filter 30 can be changed by changing b_(o) in formula (2) above. If b₁≠0, the gain of the resonance filter 30 can be changed by rearranging formula (2) above into formula (3) below, and changing b₀ in formula (3). H _(A)(s)=b ₀(1+b ₁ s/b ₀)/(s ²+2ζω_(r) s+ω _(r) ²)  (3)

FIG. 7 shows the measurement results (experimental results) of the variation range of (i_(δ)*+i_(δC)), the amplitude of a first-order component of (i_(δ)*+i_(δC)), and the amount of decrease or increase of power consumption, the measurement results being obtained when the gain of the resonance filter 30 is variously changed. In FIG. 7, the horizontal axis represents the gain of the resonance filter 30. For polygonal lines 221 and 222, the vertical axis represents the current value; for a polygonal line 223, the vertical axis represents the amount of decrease or increase of power consumption. In the following description, what is referred to simply as the “gain” always refers to that of the resonance filter (in this example, the resonance filter 30). In addition, what is referred to simply as the “power consumption” always refers to that of the motor drive system according to an embodiment.

In the experiment corresponding to FIG. 7, the gain of the resonance filter 30 was changed in nine levels. The nine levels of gain are referred to, in order of increasing gain, as G₁, G₂, G₃, G₄, G₅, G₆, G₇, G₈, and G₉. In addition, G₁ is zero. That is, if the gain is G₁, the resonance filter 30 is practically nonexistent.

The polygonal line 221 shows the experimental result indicating the gain dependence of the variation range of (i_(δ)*+i_(δC)). The variation range of (i_(δ)*+i_(δC)) is the difference (in this case, the difference is a positive value) between the minimum and maximum values of (i_(δ)*+i_(δC)) observed while the motor 1 rotates one-turn in mechanical angle. The polygonal line 222 shows the experimental result indicating the gain dependence of the amplitude of the first-order component of (i_(δ)*+i_(δC)). The amplitude of the first-order component of (i_(δ)*+i_(δC)) is the amplitude of a frequency component of ω_(r) of (i_(δ)*+i_(δC)). The polygonal line 223 shows the experimental result indicating the gain dependence of the amount of decrease or increase of power consumption relative to power consumption observed when the gain is zero (that is, b_(o)=0). It is to be noted that the experiments corresponding to the polygonal lines 221 to 223 were performed with the conditions (such as b₁ and ω*) other than gain fixed at constant values.

As will be understood from FIG. 7, as the gain increases from G₁ to G₄, the variation range of (i_(δ)*+i_(δC)) and the amplitude of the first-order component of (i_(δ)*+i_(δC)) decrease due to the effect of superimposition of the corrected δ-axis current value i_(δC). The variation range of (i_(δ)*+i_(δC)) and the amplitude of the first-order component of (i_(δ)*+i_(δC)) reach a minimum value at gain G₄. Then, as the gain further increases from G₄ to G₉, the variation range of (i_(δ)*+i_(δC)) and the amplitude of the first-order component of (i_(δ)*+i_(δC)) increase.

The amount of decrease or increase of power consumption behaves in a similar way. That is, as the gain increases from G₁ to G₄, power consumption decreases. The power consumption reaches a minimum value at gain G₄. Then, as the gain further increases from G₄ to G₉, the power consumption gradually increases from this minimum value. These experimental results revealed that, although a higher gain contributes to a greater vibration-reduction effect, too high a gain is undesirable from the viewpoint of reducing power consumption.

FIGS. 8 and 9 show FFT (fast Fourier transform) analysis results of (i_(δ)*+i_(δC)) corresponding to the experiments shown in FIG. 7. In FIGS. 8 and 9, the horizontal axis represents the order, and the vertical axis represents the amplitude of each order component. FIG. 9 is an enlarged view of zeroth- and first-order parts of FIG. 8. In FIG. 8, bar groups marked with reference numerals 250, 251, 252, 253, 254, 255, 256, 257, 258, and 259 respectively represent the amplitudes of zeroth-, first-, second-, third-, fourth-, fifth-, sixth-, seventh-, eighth-, and ninth-order components of (i_(δ)*+i_(δC)). The zeroth-order component of (i_(δ)*+i_(δC)) is a direct current component of (i_(δ)*+i_(δC)), and the jth-order component (where j is an integer from 1 to 9) of (i_(δ)*+i_(δC)) is a frequency component of (ω_(r)×j) of (i_(δ)*+i_(δC)).

Each bar group consists of nine bars. In each bar group, the height of the leftmost bar represents the amplitude observed when the gain is zero, and the gain becomes higher toward the right side. That is, in FIG. 9, the heights of bars 271, 272, 273, 274, 275, 276, 277, 278, and 279 respectively represent the amplitudes of the zeroth-order component of (i_(δ)*+i_(δC)) observed when the gain is G₁, G₂, G₃, G₄, G₅, G₆, G₇, G₈, and G₉, and the heights of bars 281, 282, 283, 284, 285, 286, 287, 288, and 289 respectively represent the amplitudes of the first-order component of (i_(δ)*+i_(δC)) observed when the gain is G₁, G₂, G₃, G₄, G₅, G₆, G₇, G₈, and G₉.

These figures show the following points. As the gain increases from G₁ to G₄, the amplitude of the first-order component of (i_(δ)*+i_(δC)) decreases. The amplitude of the first-order component of (i_(δ)*+i_(δC)) reaches a minimum value at gain G₄. Then, as the gain further increases from G₄ to G₉, the amplitude increases. In addition, the amplitude of the zeroth-order component of (i_(δ)*+i_(δC)) changes little despite variations in gain, and the amplitude of a second- and higher order component is considerably small as compared with the amplitudes of the zeroth- and first-order components.

Since the main cause for variations in torque-related δ-axis current is variations in load torque, and the frequency of the variations is ω_(r), the power consumption is considered to be minimized by minimizing the amplitude of the first-order component of (i_(δ)*+i_(δC)).

Although the power consumption is most strongly influenced by the direct current component of (i_(δ)*+i_(δC)), as is clear from FIGS. 8 and 9, the direct current component (zeroth-order component) of (i_(δ)*+i_(δC)) changes little despite variations in gain. In addition, since the amount of variations in frequency components of (i_(δ)*+i_(δC)) other than the first-order component is small, variations in the first-order component is the dominant factor in variations in (i_(δ)*+i_(δC)) itself, which corresponds to a product obtained by combining all the order components. As a result, a gain at which the amplitude of the first-order component of (i_(δ)*+i_(δC)) is minimized is in general considered to be identical to a gain at which the variation range of (i_(δ)*+i_(δC)) is minimized. Therefore, minimization of power consumption may be achieved by minimizing the variation range of (i_(δ)*+i_(δC)), instead of minimizing the amplitude of the first-order component of (i_(δ)*+i_(δC)).

In general, i_(γ)*=0 and is >>i_(γ), and a power loss of the motor drive system is roughly proportional to the square of the δ-axis current i_(δ) (≈i_(δ)*+i_(δC)). Suppose a direct current component of is constant. Then, as is clear from a general relational expression (4), power consumption is minimized when is has only a direct current component, and power consumption increases with an increase in the variation range of is (strictly speaking, however, power consumption is also influenced by a phase relationship between voltage and current). Thus, by minimizing the variation range of (i_(δ)*+i_(δC)) or the amplitude of the first-order component of (i_(δ)*+i_(δC)), it is possible to minimize power consumption.

$\begin{matrix} {{\int_{0}^{2\;\pi}{1^{2}\ {\mathbb{d}x}}} < {\int_{0}^{2\;\pi}{\left( {1 + {\sin\; x}} \right)^{2}{\mathbb{d}x}}}} & (4) \end{matrix}$

The above-described method for minimizing power consumption is applied to the motor control device 3 a shown in FIG. 3. Specifically, the gain controller 32 shown in FIG. 3 calculates a gain (that is, a gain coefficient b₀) of the resonance filter 30 by referring to (i_(δ)*+i_(δC)) outputted from the adder 31, such that the variation range of (i_(δ)*+i_(δC)) or the amplitude of the first-order component of (i_(δ)*+i_(δC)) is minimized. The resonance filter 30 calculates the corrected δ-axis current value i_(δC) by using the gain thus calculated, and outputs the corrected δ-axis current value i_(δC).

A method for minimizing the variation range of (i_(δ)*+i_(δC)) will be explained with reference to FIG. 10. FIG. 10 is a flow chart showing the procedure for minimizing the variation range of (i_(δ)*+i_(δC)). This procedure is based on a so-called hill-climbing algorithm.

At the time of execution of this procedure, the most current value of (i_(δ)*+i_(δC)) is successively assigned to a variable i_(δ)Com. In addition, a variable i_(δ)ComMax to which a maximum value of i_(δ)Com is assigned and a variable i_(δ)ComMin to which a minimum value of i_(δ)Com is assigned are adopted, and a variable i_(δ)Amp_now to which the variation range of the current i_(δ)Com is assigned and a variable i_(δ)Amp_old to which the variation range of the last i_(δ)Com is assigned are adopted. Furthermore, G is adopted as a variable representing a gain (that is, a gain coefficient b₀) of the resonance filter 30. The amount of change in variable G per change is α. The initial values of the variables i_(δ)ComMax, i_(δ)ComMin, i_(δ)Amp_now, and i_(δ)Amp_old are set at zero. The initial value of the variable G is set at a predetermined value.

Steps S11 to S20 are performed every time the variable i_(δ)Com is updated by the gain controller 32. First, in step S11, it is checked whether or not the rotor of the motor 1 has rotated one-turn from a given base point in time. Here, rotating “one-turn” is not rotating one-turn in electrical angle but rotating one-turn in mechanical angle. If the rotor of the motor 1 is found not to have rotated one-turn, the procedure proceeds to step S12, and it is checked whether or not the current variable i_(δ)Com is greater than the current variable i_(δ)ComMax. If i_(δ)Com>i_(δ)ComMax, the procedure proceeds to step S14. In step S14, the current variable i_(δ)Com is assigned to the variable i_(δ)ComMax, and the procedure proceeds to step S13. On the other hand, if i_(δ)Com≦i_(δ)ComMax, the procedure directly proceeds to step S13.

In step S13, it is checked whether or not the current variable i_(δ)Com is smaller than the current variable i_(δ)ComMin. If i_(δ)Com<i_(δ)ComMin, the procedure proceeds to step S15. In step S15, the current variable i_(δ)Com is assigned to the variable i_(δ)ComMin, and the procedure goes back to step S11. On the other hand, if i_(δ)Com≧i_(δ)ComMin, the procedure directly goes back to step S11.

In step S11, if the rotor of the motor 1 is found to have rotated one-turn from the base point in time, the procedure proceeds to step S16. At this point, the maximum and minimum values of the variable i_(δ)Com obtained during one turn of the rotor are assigned to the variables i_(δ)ComMax and i_(δ)ComMin, respectively. In step S16, (i_(δ)ComMax−i_(δ)ComMin) is assigned to the variable i_(δ)Ampnow. Then, in step S17, it is checked whether or not an inequality i_(δ)Amp_now<i_(δ)Amp_old holds. If this inequality is found to hold, the procedure directly proceeds to step S19. On the other hand, if this inequality is found not to hold, the procedure proceeds to step S18, and a value obtained by multiplying the current variable α by −1 is newly assigned to the variable α. Then, the procedure proceeds to step S19.

In step S19, a variable α is added to the current variable G, and α value thus obtained serves as a new variable G. The variable G thus updated is transmitted to the resonance filter 30, and is used as a gain coefficient b₀ when calculating the corrected δ-axis current value i_(δC). Thereafter, in step S20, zero is assigned to the variable i_(δ)ComMax, a maximum value MAX of the variable i_(δ)ComMin is assigned to the variable i_(δ)ComMin, and a value of the current variable i_(δ)Amp_now is assigned to the variable i_(δ)Amp_old. Then, the procedure goes back to step S12. It is assumed that the variable i_(δ)ComMin takes on various values. The maximum value MAX here is the maximum of the various values that the variable i_(δ)ComMin is assumed to take on. A time point at which the procedure goes back from step S20 to step S12 serves as a base point in time used as the reference for the next branching process in step S11.

By repeatedly performing a loop process consisting of steps S11 to S20, the variation range of (i_(δ)*+i_(δC)) is kept at or near a minimum value (local minimum, to be exact).

The procedure for minimizing the variation range of (i_(δ)*+i_(δC)) has been explained by using FIG. 10. Needless to say, however, the amplitude of the first-order component of (i_(δ)*+i_(δC)) may be minimized instead by using a similar method. In that case, it is necessary simply to extract the first-order component of (i_(δ)*+i_(δC)) from the output value of the adder 31 by using FFT (fast Fourier transform), and sequentially adjust the variable G such that the amplitude of the first-order component is kept at or near a minimum value.

In the configuration described in JP-A-2006-180605, to achieve a reduction in power consumption requires the following processes. First, power consumption is sequentially measured while changing a limit value to a current component for correcting a torque variation component, and an optimum limit value is determined in advance based on the measurement results. Then, the optimum limit value thus obtained is stored as table data, and is referred to at the time of actual operation. Such an adjustment operation for deriving a parameter (limit value) is complicated. By contrast, the motor control device 3 a makes it possible to automatically minimize power consumption without the need for performing such an adjustment operation, and at the same time reduce vibration and noise.

Example 2

Next, Example 2 of the invention will be described. FIG. 11 is a detailed block diagram of a motor drive system according to Example 2. The motor drive system shown in FIG. 11 includes the motor 1 and the inverter 2, which are shown in FIG. 1, a motor control device 3 b serving as the motor control device 3 shown in FIG. 1, and the phase-current sensor 11. The motor control device 3 b includes different parts designated with reference numerals 12 to 20 and 30 to 32. The motor control device 3 b can be considered to include the phase-current sensor 11. The different parts constituting the motor control device 3 b can freely use all the values produced within the motor control device 3 b.

In the motor control device 3 a shown in FIG. 3, the resonance filter 30 receives a speed deviation (ω*−ω_(e)) as an input signal. However, in the motor control device 3 b shown in FIG. 11, the resonance filter 30 receives, as an input signal, the specified δ-axis current value is from the speed controller 17 instead of a speed deviation (ω*−ω_(e)). Thus, in this example, the resonance filter 30 extracts from i_(δ)* a periodic variation component resulting from variations in load torque, and outputs the variation component thus extracted to the adder 31 as i_(δC). The motor control devices 3 a and 3 b differ only in the input signal of the resonance filter 30; in other respects, they are identical with each other.

In a case where the speed deviation (ω*−ω_(e)) varies due to variations in load torque, the specified δ-axis current value i_(δ)* also varies in a similar manner in synchronism with the speed deviation (ω*−ω_(e)). Therefore, with the configuration of the motor control device 3 b, it is possible to achieve the same effects as those achieved in Example 1.

Example 3

Next, Example 3 of the invention will be described. FIG. 12 is a detailed block diagram of a motor drive system according to Example 3. The motor drive system shown in FIG. 12 includes the motor 1 and the inverter 2, which are shown in FIG. 1, a motor control device 3 c serving as the motor control device 3 shown in FIG. 1, and the phase-current sensor 11. The motor control device 3 c includes different parts designated with reference numerals 12 to 20, 31, and 32, and a resonance filter 30 c. The motor control device 3 c can be considered to include the phase-current sensor 11. The different parts constituting the motor control device 3 c can freely use all the values produced within the motor control device 3 c.

In the motor control device 3 a shown in FIG. 3, the resonance filter 30 calculates the corrected δ-axis current value i_(δC) from the speed deviation (ω*−ω_(e)). However, in the motor control device 3 c shown in FIG. 12, the resonance filter 30 c calculates the corrected δ-axis current value i_(δC) from the axis error Δθ. The motor control devices 3 a and 3 c differ only in the resonance filter; in other respects, they are identical with each other. In the following description, only the resonance filter 30 c and input and output thereof are explained, and the explanations of such parts as are found in both the motor control devices 3 a and 3 c will be omitted.

The resonance filter 30 c receives the axis error Δθ estimated by the position/speed estimator 20 as an input signal, and extracts from the axis error Δθ a periodic variation component resulting from variations in load torque. Then, the resonance filter 30 c outputs the variation component thus extracted as a corrected δ-axis current value i_(δC). The transfer function H_(B)(S) of the resonance filter 30 c is given by formula (5) below. H _(B)(s)=(b ₀ s+b ₁)/(s ²+2ζω_(r) s+ω _(r) ²)  (5)

Here, b_(o) represents a gain coefficient, b, represents a phase adjusting value, ζ represents an attenuation coefficient, and (Or represents a natural angular frequency, and these symbols are the same as those described in Example 1. In addition, s represents the Laplace operator. The resonance filter 30 c amplifies (emphasizes) a frequency component of ω_(r) of the input signal to a degree commensurate with the gain coefficient b_(o), and outputs it. Ideally, the resonance filter 30 c extracts only a frequency component of ω_(r) of the input signal, and outputs it.

Since the axis error Δθ varies in synchronism with periodic variations in load torque, a periodic variation component of the axis error Δθ is emphasized in i_(δC) obtained by multiplying the axis error Δθ by the transfer function H_(B)(s). Here, the degree of emphasis, that is, the gain of the resonance filter 30 c, is determined by the gain coefficient b_(o).

In the motor control device 3 c, the adder 31 calculates the sum (i_(δ)*+i_(δC)) of the specified δ-axis current value i_(δ)* from the speed controller 17 and the corrected δ-axis current value i_(δC) from the resonance filter 30 c, and outputs it to the subtracter 13. As in Example 1, the gain controller 32 adjusts the gain (that is, the gain coefficient b_(o) in formula (5)) of the resonance filter 30 c based on the output value (i_(δ)*+i_(δC)) of the adder 31, such that the variation range of (i_(δ)*+i_(δC)) or the amplitude of the first-order component of (i_(δ)*+i_(δC)) is minimized. As a result, it is possible to achieve the same effects as those achieved in Example 1.

In the motor control device 3 c shown in FIG. 12, the axis error Δθ is inputted to the resonance filter 30 c. However, a value of any other type may be inputted to the resonance filter 30 c as long as it varies in synchronism with variations in the axis error Δθ (variations in the axis error Δθ at a natural angular frequency (or), because the value varying in synchronism with variations in the axis error Δθ contains, as is the case with the axis error Δθ, a periodic variation component synchronized with periodic variations in load torque.

For example, a signal that is proportional (or substantially proportional) to the axis error Δθ may be inputted to the resonance filter 30 c.

For example, a torque variation component ΔTm estimated by using the axis error Δθ may be inputted to the resonance filter 30 c as an input signal. As described in the treatise titled “Reduction Control Method of Periodic Torque Disturbance for Compressor” by Yasuo Notohara et al.; presented at the 2004 Annual Conference of the Industry Applications Society of the Institute of Electrical Engineers of Japan; 1-57 (1-337-I-340); Sep. 14, 2004, since the torque variation component ΔTm is an approximate value calculated by, for example, formula (6) below, it can be considered to be proportional to the axis error Δθ. In formula (6), P represents the number of poles of the motor 1, and J represents inertia.

$\begin{matrix} {{\Delta\;{Tm}} = {\frac{2J\;\omega_{r}^{2}}{P} \cdot {\Delta\theta}}} & (6) \end{matrix}$

The torque variation component ΔTm corresponds to the result of subtraction of a load torque from a torque produced by the motor 1, and the torque produced by the motor 1 cannot follow periodic variations in load torque, causing torque variations to occur (that is, preventing ΔTm from becoming zero). The torque variation component ΔTm causes variations in speed, resulting in variations in the axis error Δθ.

Example 4

Examples 1 to 3 deal with the motor drive systems in which vector control is performed such that the axis error Δθ between the d-axis and the γ-axis is made to converge to zero, that is, such that the γ-axis is made to follow the d-axis; however, Examples 1 to 3 may be modified to be Example 4 in which vector control is performed such that the γ-axis is made to follow an axis other than the d-axis. For example, by defining a dm-axis described in the treatise titled “Position Sensorless Vector Control for Permanent Magnet Synchronous Motors Based on Maximum Torque Control Frame” by Hida et al.; published by the Industry Applications Society of the Institute of Electrical Engineers of Japan; included in the Collection of the Lecture Treatises Presented at the 2006 Annual Conference of the Industry Applications Society of the Institute of Electrical Engineers of Japan; pp. 385-388 (I-385-I-388); August 2006, vector control may be performed such that the γ-axis is made to follow the dm-axis.

The dm-axis is an axis that lags behind a qm-axis by an electrical angle of 90 degrees. The qm-axis is the rotation axis whose direction coincides with that of the current vector to be fed to the motor 1 when maximum torque control is achieved. The current vector to be fed to the motor 1 is the current to be fed to the motor 1, the current being expressed in vector form. Alternatively, the qm-axis may be the rotation axis having a phase leading the rotation axis whose direction coincides with that of the current vector to be fed to the motor 1 when maximum torque control is achieved.

In a case where vector control is performed such that the γ-axis is made to follow the dm-axis, it is necessary simply to perform the following processing, for example. The position/speed estimator 20 shown in FIG. 3 and other drawings estimates the axis error Δθ_(m) between the dm-axis and the γ-axis by using all or part of i_(γ), i_(δ), v_(γ)* and v_(δ)*, and estimates the rotor position θ_(e) and the rotation speed ω_(e) such that the axis error Δθ_(m) is made to converge to zero by using proportional-plus-integral control.

Example 5

Examples 1 to 4 deal with the motor drive systems in which position sensorless vector control is performed that uses no position sensor for detecting the rotor position. However, the techniques described in Examples 1 to 4 are useful in a case where the position sensor is provided. As Example 5 of the invention, a description will be given below of a motor drive system provided with the position sensor. Any feature of Examples 1 to 4 can be applied, unless inconsistent, to Example 5.

For the sake of concreteness, with reference to FIG. 3, a configuration (unillustrated) of a motor drive system that differs from the motor drive system shown in FIG. 3 according to Example 1 in that a position sensor is further added will be described. The motor drive system according to Example 5 differs from the motor drive system shown in FIG. 3 in that θ_(e) and ω_(e) are detected based on the output signal of the position sensor, and that this eliminates the need for the estimator 20. In other respects, this motor drive system is the same as that shown in FIG. 3.

The position sensor is realized with, for example, Hall devices or resolvers, and outputs a signal for specifying the magnetic pole position of the permanent magnet 1 a of the rotor of the motor 1 (that is, a signal for specifying the rotor position θ). The phase of the d-axis, relative to the U-phase armature winding fixed axis, is detected based on the output signal of the position sensor. The phase (rotor position) thus detected is treated as θ_(e). This rotor position θ_(e) is, ideally, identical to θ shown in FIG. 2, and is fed to the coordinate converters 12 and 18. In addition, the rotor position θ_(e) is differentiated by a speed calculating differentiator (unillustrated) to obtain ω_(e), and ω_(e) thus obtained is fed to the subtracter 19 and the current controller 15.

It is needless to say that the same effects as those achieved in Example 1 can be achieved by configuring the motor drive system as in Example 5.

Example 6

As an example of an apparatus to which the motor drive systems described in Examples 1 to 5 are applied, a compressor 400 is shown in FIG. 13. FIG. 13 is an external view of the compressor 400. Any one of the motor drive systems according to Examples 1 to 5 is provided in the compressor 400. The compressor 400 compresses refrigerant gas (unillustrated) by using a torque of the motor 1 (a torque produced by the motor 1) as its drive source.

For example, the compressor 400 is a scroll compressor. In this case, a pair of scrolls (unillustrated) of identical shape are provided inside the compressor 400. One of the scrolls is fixed, and the other is made to orbit eccentrically by a torque of the motor 1. This changes the volume of the compression space, whereby gases (such as refrigerant gas) inside the compression space are compressed. Before and after the compression of the gas, sucking and discharge of the gas is performed. In this case, a load that is directly driven by the torque of the motor 1 is the scroll. However, the scroll compressor itself can be considered to be a load of the motor 1.

Needless to say, the compressor 400 may be a compressor other than a scroll compressor, such as a reciprocating compressor or a rotary compressor. In a case where the compressor 400 is a reciprocating compressor, the compressor 400 has a piston and a cylinder forming a compression space, and the piston is made to reciprocate in the cylinder by the torque of the motor 1. This changes the volume of the cylinder, whereby gases (such as refrigerant gas) inside the cylinder are compressed. In this case, a load that is directly driven by the torque of the motor 1 is the piston. However, the reciprocating compressor itself can be considered to be a load of the motor 1.

Example 7

The behavior of power consumption described above will be explained by using theoretical formulae. The following explanation is provided as an explanation of Example 7.

Let power consumption of the motor drive system be P_(W). Then, the power consumption Pw is given by formula (7a) below. Assuming that i_(d) is ignored because, in general, i_(d)=0 or i_(q)>>i_(d)≠0, then the power consumption Pw is given by formula (7b). Here, v_(d) and v_(q) represent the d-axis component and the q-axis component, respectively, of the motor voltage V_(a), and i _(d) and i_(q) represent the d-axis component and the q-axis component, respectively, of the motor current I_(a). P _(W) =i _(d) v _(d) +i _(q) v _(q)  (7a) P _(W) =i _(q) v _(q)  (7b)

In addition, the voltage equation of the permanent-magnet synchronous motor is given by formula (8a). Rearranging formula (8a) gives formula (8b). Furthermore, assuming that i_(d)≈0 and the system is in a steady state, then the derivative term can be ignored. As a result, formula (8c) holds. Here, Φ_(a) represents the armature flux linkage ascribable to the permanent magnet of the motor 1, and p represents a differential operator.

$\begin{matrix} {\begin{bmatrix} v_{d} \\ v_{q} \end{bmatrix} = {{\begin{bmatrix} {R_{a} + {pL}_{d}} & {{- \omega}\; L_{q}} \\ {\omega\; L_{d}} & {R_{a} + {pL}_{q}} \end{bmatrix}\begin{bmatrix} i_{d} \\ i_{q} \end{bmatrix}} + \begin{bmatrix} 0 \\ {\omega\;\Phi_{a}} \end{bmatrix}}} & \left( {8a} \right) \\ {v_{q} = {{\omega\; L_{d}i_{d}} + {\left( {R_{a} + {p\; L_{q}}} \right)i_{q}} + {\omega\Phi}_{a}}} & \left( {8b} \right) \\ {v_{q} = {{R_{a}i_{q}} + {\omega\Phi}_{a}}} & \left( {8c} \right) \end{matrix}$

Substituting formula (8c) in formula (7b) gives formula (9). P _(W) =R _(a) i _(q) ²+ωΦ_(a) i _(q)  (9)

The first term in the right side of formula (9) represents a power loss due to the motor resistance, and the second term in the right side thereof represents power involved in the occurrence of torque. Due to the presence of the first term that is proportional to i_(q) ², an increase in the harmonic components contained in i_(q) leads to an increase in loss and hence in power consumption. In a case where the γ-δ axes is made to follow the d-q axes as in Example 1, since i_(q) follows (i_(δ)*+i_(δC)), by reducing the harmonic components (in particular, the first-order component which is the most dominant of them all) of (i_(δ)*+i_(6C)), it is possible to reduce power consumption.

Now, let the waveform of i_(δ)* be fi given by formula (10a), and the waveform of i_(δC) be fr given by formula (10b). Here, A₁ and A₂ represent an amplitude value of the waveform fi and an amplitude value of fr, respectively, CONST represents a constant, and Q represents the phase of the waveform fr, satisfying π/2≦Q≦π. In addition, t represents time. fi=A ₁ sin(ωt)+CONST  (10a) fr=A ₂ sin(ωt+Q)  (10b)

If an amplitude value A₂ is increased from zero, the amplitude of the combined waveform (fi+fr) first decreases and then increases. The simulation result showing how the amplitude of the combined waveform (fi+fr) depends on an amplitude value A₂ is indicated by a curve 410 in FIG. 14. In the graph showing the curve 410, the horizontal axis represents an amplitude value A₂, and the vertical axis represents the amplitude of (fi+fr). In this simulation, the amplitude of (fi+fr) was estimated, assuming that A₁=10, ω=30, CONST=20, and Q=2π·100/360, and changing A₂ from 0 to 10 (the unit of each value is omitted).

As described above, there is an amplitude value A₂ that minimizes the amplitude of (fi+fr), and reducing the amplitude of (fi+fr) also helps reduce power consumption. That is, there is a gain of the resonance filter that minimizes the amplitude (variation range) of (i_(δ)*+i_(δC)), and reducing the amplitude of (i_(δ)*+i_(δC)) also helps reduce power consumption while reducing vibration.

Modifications and Variations

What has been explained about an example can be applied, unless inconsistent, to any other example. At the time of application, it can be construed, if necessary, that the difference among reference numerals (such as 3 a, 3 b, and 3 c) attached to the parts having the same name may be ignored. Hereinafter, notes 1 to 4 will be described as modified examples of the embodiment described above or annotations made thereon. Any feature of notes 1 to 4 described below can be applied, unless inconsistent, to any note other than that in connection with which the feature is specifically described.

Note 1

Any of the different specified values (such as i_(γ)*, i_(δ)*, v_(γ)*, and v_(δ)*) and state quantities (such as i_(γ) and i_(δ)) mentioned above, that is, any value that needs to be derived as necessary may be derived in any manner. That is, such values may be derived, for example, through calculation performed within the motor control device (3 a, 3 b, or 3 c), or may be derived from a previously set table data.

Note 2

The embodiment described above deals with a case in which the U-phase current i_(u) and the V-phase current i_(v) are directly detected by using the phase-current sensor 11; however, it is also possible to detect them based on the direct current on the power supply side of the inverter 2.

Note 3

Part or all of the functions of the motor control device (3 a, 3 b, or 3 c) is realized, for example, with software (program) incorporated in a general-purpose microcomputer or the like. When the motor control device is realized with software, the block diagrams showing the configurations of different parts of the motor control device serve as functional block diagrams. Needless to say, the motor control device may be realized with hardware alone, instead of software (program), or may be realized with a combination of software and hardware.

Note 4

For example, it can be considered that, in the embodiment described above, the position/speed estimator 20 shown in FIG. 3 and other drawings serves as a motor speed deriving portion that derives the motor speed ω_(e) by estimation. However, in Example 5, the aforementioned speed calculating differentiator (unillustrated) serves as the motor speed deriving portion, and this speed calculating differentiator detects the motor speed ω_(e) in collaboration with the position sensor (the motor speed deriving portion may be considered to include the position sensor).

Since the specified δ-axis current value is a specified value for a current component related to the torque of the motor 1, it can be called a specified torque current value. In response to this, the corrected δ-axis current value i_(δC) can be called a corrected torque current value. In addition, the gain controller 32 shown in FIG. 3 and other drawings serves as an adjusting portion that adjusts the gain of the resonance filter (30 or 30 c), and the adder 31 shown in FIG. 3 and other drawings serves as a torque current corrector. 

1. A motor control device performing vector control for a motor that drives a load whose load torque varies periodically, the motor control device comprising: a motor speed deriving portion estimating or detecting a motor speed; a speed controller producing a specified torque current value such that the motor speed is made to follow a specified motor speed value fed from outside; a resonance filter producing a corrected torque current value by receiving a control value that varies with variations in the load torque and emphasizing a periodic variation component of the control value; a torque current corrector producing a specified superimposed torque current value by superimposing the corrected torque current value on the specified torque current value; and an adjusting portion adjusting, based on the specified superimposed torque current value, a degree of emphasis placed on the variation component by the resonance filter, wherein the vector control is performed according to the specified superimposed torque current value.
 2. The motor control device of claim 1, wherein the control value is a difference between the motor speed and the specified motor speed value, or the control value is the specified torque current value.
 3. The motor control device of claim 1, wherein, let an axis parallel to a magnetic flux produced by a permanent magnet provided on a rotor of the motor be called a d-axis, and let an axis estimated for control purposes, the axis corresponding to the d-axis, be called a γ-axis, then, the motor control device comprises an estimator estimating, based on a motor current to be fed to the motor, an axis error between the d-axis and the γ-axis, and the motor speed, wherein the control value is the axis error, or a value varying in synchronism with variations in the axis error.
 4. The motor control device of claim 1, wherein the adjusting portion adjusts the degree of emphasis based on a variation range of the specified superimposed torque current value.
 5. The motor control device of claim 4, wherein the adjusting portion adjusts the degree of emphasis such that the variation range is reduced.
 6. The motor control device of claim 1, wherein the adjusting portion extracts, from the specified superimposed torque current value, a frequency component of variations in the load torque, and adjusts the degree of emphasis based on an amplitude of the frequency component.
 7. The motor control device of claim 6, wherein the adjusting portion adjusts the degree of emphasis such that the amplitude of the frequency component is reduced.
 8. A motor drive system, comprising: a motor; an inverter driving the motor; and the motor control device of claim 1 performing vector control for the motor via the inverter.
 9. A compressor using, as a drive source thereof, a torque of the motor provided in the motor drive system of claim
 8. 